Introduction to NeXL

What is NeXL?

NeXL is a collection of packages (libraries) for the Julia language that implement common X-ray microanalysis algorithms, physical data and utilities.

The core NeXL packages are

• NeXLCore - Defines core concepts like elements, X-rays, atomic shells, k-ratios and fundamental electron and X-ray algorithms.
• NeXLMatrixCorrection - Implements algorithms for performing matrix correction for bulk samples
• NeXLSpectrum - Implements data types and algorithms to handle spectra and hyper-spectra

NeXL builds on many packages from the Julia infrastructure including

• Gadfly - A "grammar of graphics" plotting package
• DataFrames - "Pandas-like" tools for working with tabular data

Why Julia?

Julia is a high-performance scripting language designed for numerical data analysis. The base Julia libraries provide basic scalar, vector and matrix numerical analysis tools. Julia differs from most scriptable languages in that all code is compiled before execution. This leads to a "slow then fast" user experience. The first time a method is used, it and all the methods it depends upon must be compiled. This can lead to a significant delay. However, once compiled, the code is fast - often as fast as C or Fortran code. You will notice this "slow then fast" nature as you work with this notebook. It is particularly evident when creating plots.

NeXLCore

We will start by exploring NeXLCore since this package provides core functionality for the other NeXL packages.

using DrWatson
@quickactivate "IUMAS"

using NeXLCore

  Activating project at `c:\Users\nritchie\Desktop\IUMAS`

Elements

We will first construct a datum representing an element and then manipulate this object to extract elemental data.

Julia is not an object-oriented language. Instead it uses what is called "multiple dispatch" to determine which method implementation to call dependent on the arguments handed to the function.

el = n"Tc"  # Here we are using a special syntactic sugar to convert the string "Tc" into an datum

Technetium (Tc), number 43:

category	transition metal
atomic mass	98.0 u
density	11.0 g/cm³
molar heat	24.27 J/mol⋅K
melting point	2430.0 K
boiling point	4538.0 K
phase	Solid
shells	[2, 8, 18, 13, 2]
electron configuration	1s² 2s² 2p⁶ 3s² 3p⁶ 4s² 3d¹⁰ 4p⁶ 5s² 4d⁵
appearance	shiny gray metal
summary	Technetium (/tɛkˈniːʃiəm/) is a chemical element with symbol Tc and atomic number 43. It is the element with the lowest atomic number in the periodic table that has no stable isotopes:every form of it is radioactive. Nearly all technetium is produced synthetically, and only minute amounts are found in nature.
discovered by	Emilio Segrè
source	https://en.wikipedia.org/wiki/Technetium

Let's get some properties of this elemental datum.

z(el), a(el), symbol(el), name(el)

(43, 98.0, "Tc", "Technetium")

We can combine elements into materials. The mat"..." macro converts expressions into Material structs.

mat = mat"Ca(PO4)3OH"
mat, typeof(mat)

(Ca(PO4)3OH[P=0.2717,Ca=0.1172,O=0.6082,H=0.0029], Material{Float64, Float64})

An alternative syntax allows you to specify additional properties of the Material.

mat = parse(Material, "Ca(PO4)3OH", name = "Apatite", density = 2.2)

Apatite[P=0.2717,Ca=0.1172,O=0.6082,H=0.0029,2.20 g/cm³]

In addition to being able to parse chemical formulae, NeXLCore can also parse expressions like the next one. In this case, the multiplier represents the mass fraction of the element. The right hand side can also be a chemical formula as though the material was made from various mass fractions of consituent materials.

adm = parse(Material, "0.3399*O+0.0664*Al+0.0405*Si+0.0683*Ca+0.0713*Ti+0.1055*Zn+0.3037*Ge", name="ADM-6005a")

ADM-6005a[Ti=0.0713,Al=0.0664,Ge=0.3037,Ca=0.0683,Zn=0.1055,O=0.3399,Si=0.0405]

In addition to elements and materials, NeXLCore provides mechanisms to work with characteristic X-rays, atomic shells and other atomic physics data. The n"..." macro can be used to create Element, CharXRay, AtomicSubShell and SubShell structs.

cxr = n"Tc K-L3"
cxr, typeof(cxr)

(Tc K-L3, CharXRay)

ass = n"Tc K"
ass, typeof(ass)

(Tc K, AtomicSubShell)

Let's get some properties of the CharXRay datum. You'll notice that the energy is in electron-volts as is the case for all energies within NeXL.

energy(cxr), inner(cxr), energy(inner(cxr)), outer(cxr), energy(outer(cxr)), typeof(inner(cxr))

(18367.0, Tc K, 21050.0, Tc L3, 2683.0, AtomicSubShell)

To determine every characteristic X-ray generated by a particular element, you can use the characteristic(...). To generate sub-sets of the transitions replace alltransitions with ktransitions, ltransitions or mtransitions.

cxrs=characteristic(el, alltransitions)
cxrs, length(cxrs)

(Tc K-L3 + 9 others, Tc L3-M5 + 23 others & Tc M5-N3 + 9 others, 44)

Now we can use various functions to extract X-ray related physical data from elements and materials. The mac(...) function returns the mass absorption coeffficient in $cm^2/g$.

mac(mat, n"Ca K-L3"), mac(n"Ca", n"Ca K-L3"), mac(mat, 3692.0), mac(n"Ca", 3692.0)

(257.51384578832244, 139.20100028283625, 257.51384578832244, 139.20100028283625)

This is an example of one of Julia's core design features - multiple dispatch. The function mac(...) is called on four distinct argument types.

• mac(Material, CharXRay)
• mac(Element, CharXRay)
• mac(Material, Float64)
• mac(Element, Float64)

This is similar but extends on the way object oriented code can use the object type to determine which function implementation to call.

NeXL uses the Gadfly library to plot spectra and other data items.

using Gadfly
plot(e->mac(mat, e), 100.0, 1.0e4, Scale.y_log10)

plot(
    layer(e->mac(mat, e), 100.0, 1.0e4, Theme(default_color="Red")),
    layer(e->mac(n"Ca", e), 100.0, 1.0e4, Theme(default_color="Green")),
    layer(e->mac(n"P", e), 100.0, 1.0e4, Theme(default_color="Blue")),
    Scale.y_log10
)

There is much more functionality in NeXLCore, but that is enought to get us started. Next let's take a look at NeXLSpectrum.

NeXLSpectrum

NeXLSpectrum defines methods for reading, writing, manipulating, plotting and fitting X-ray spectra and X-ray spectrum images ("hyperspectra").

using NeXLSpectrum

[ Info: Loading Gadfly support into NeXLSpectrum.

First, we will read a spectrum from disk using the loadspectrum(...) method. It take a filename and is able to sniff the file type for many common spectrum file formats.

sp = loadspectrum(joinpath(datadir(), "exp_raw", "ADM6005a spectra","ADM-6005a_1.msa"))

  *                                                                                                  128860.0
  *                                                                                                 
  *                                                                                                 
  *                                                                                                 
  *                                                                                                 
  *                                                                                                 
  *     *                                                                                           
  *     *                                                                                           
  *     *                                                                                           
  * ** **                                                                                           
  * ** *****        **  **                                                                          
**************************************************************************************************** 20.0 keV
Spectrum{Float64}[ADM-6005a_1, -484.20818 + 5.01716⋅ch eV, 4096 ch, 20.0 keV, unknown composition, 6.81e6 counts]

set_default_plot_size(8inch, 4inch)
specs=loadspectrum.(joinpath(datadir(), "exp_raw", "ADM6005a spectra","ADM-6005a_$i.msa") for i in 1:15)
plot(specs..., klms=[n"O", n"Al", n"Si", n"Ca", n"Ti", n"Zn", n"Ge"])

plot(specs..., klms=[n"O", n"Al", n"Si", n"Ca", n"Ti", n"Zn", n"Ge"], xmax=6.0e3)

To quantify this data, we need standard spectra. The standard spectra are preprocessed to optimize the fitting process. The spectrum files are read from disk and must contain the following properties :BeamEnergy, :LiveTime, :ProbeCurrent and :TakeOffAngle to be fit and quantified. It is possible to pre-load the standard spectra and edit the properties in the script if they are not present in the spectrum file.

path=joinpath(datadir(), "exp_raw", "ADM6005a spectra")
refs=references( [
        reference(n"O", joinpath(path, "SiO2 std.msa"), mat"SiO2"),
        reference(n"Si", joinpath(path, "SiO2 std.msa"), mat"SiO2"),
        reference(n"Al", joinpath(path, "Al std.msa"), mat"Al"),
        reference(n"Ca", joinpath(path, "CaF2 std.msa"), mat"CaF2"),
        reference(n"Ti", joinpath(path, "Ti trimmed.msa"), mat"Ti"),
        reference(n"Zn", joinpath(path, "Zn std.msa"), mat"Zn"),
        reference(n"Ge", joinpath(path, "Ge std.msa"), mat"Ge"),
    ], 132.0
)
using DataFrames
asa(DataFrame, refs)

12×9 DataFrame

Row	Spectrum	Beam Energy (keV)	Probe Current (nA)	Live Time (s)	Material	Lines	ROI	P-to-B	S-to-N
	String	Float64	Float64	Float64	Material…	Array…	UnitRang…	Float64	Float64
1	SiO2	20.0	5.0	100.0	SiO2[Si=0.4674,O=0.5326]	O K-L3 + 1 other	175:228	21.8788	4119.94
2	SiO2	20.0	5.0	100.0	SiO2[Si=0.4674,O=0.5326]	Si K-L3 + 3 others	409:491	20.0938	8705.35
3	Al	20.0	5.0	100.001	Al[Al=1.0000]	Al K-L3 + 3 others	360:433	19.8537	14014.8
4	CaF2	20.0	2.5	100.0	CaF2[Ca=0.5133,F=0.4867]	Ca K-L3 + 3 others	788:938	19.4466	5767.9
5	Ti	20.0	5.0	100.001	Ti[Ti=1.0000]	Ti L3-M5 + 13 others	153:226	4.7057	1092.39
6	Ti	20.0	5.0	100.001	Ti[Ti=1.0000]	Ti K-L3 + 3 others	948:1125	22.533	10719.4
7	Zn	20.0	5.0	100.002	Zn[Zn=1.0000]	Zn L3-M5 + 13 others	247:348	17.6177	9149.2
8	Zn	20.0	5.0	100.002	Zn[Zn=1.0000]	Zn K-L3 + 1 other	1753:1882	13.61	4272.31
9	Zn	20.0	5.0	100.002	Zn[Zn=1.0000]	Zn K-M3 + 3 others	1945:2065	2.6177	686.219
10	Ge	20.0	5.0	100.001	Ge[Ge=1.0000]	Ge L3-M5 + 15 others	277:397	14.9005	9088.97
11	Ge	20.0	5.0	100.001	Ge[Ge=1.0000]	Ge K-L3 + 1 other	1997:2135	10.5729	3025.67
12	Ge	20.0	5.0	100.001	Ge[Ge=1.0000]	Ge K-M3 + 5 others	2223:2358	1.93878	478.809

The references are then used to fit the unknown spectra and matrix correction is performed. The quantify(...) method can be used to perform both operations or the fit_spectrum(...) method can be used to fit the references to the unknowns to produce k-ratios and then the k-ratios fed to the quantify(...) method to perform matrix correction. The later two-step process is useful when you want to access the k-ratio data.

qrs=map(sp->quantify(sp, refs),specs)
qdf=asa(DataFrame, qrs, nominal=adm)

16×9 DataFrame

Row	Material	O	Al	Si	Ca	Ti	Zn	Ge	Total
	String	Abstract…	Abstract…	Abstract…	Abstract…	Abstract…	Abstract…	Abstract…	Abstract…
1	ADM-6005a_1	0.380759	0.0680223	0.0388277	0.0639499	0.0733595	0.114264	0.318852	1.05803
2	ADM-6005a_2	0.379643	0.0678927	0.0389075	0.0639314	0.0728992	0.114022	0.319517	1.05681
3	ADM-6005a_3	0.381752	0.0680904	0.0387023	0.0640476	0.0730505	0.114183	0.317511	1.05734
4	ADM-6005a_4	0.38067	0.068038	0.0389573	0.0637997	0.073006	0.114154	0.31897	1.05759
5	ADM-6005a_5	0.380851	0.0683536	0.0386646	0.0640086	0.0730713	0.114185	0.317727	1.05686
6	ADM-6005a_6	0.381398	0.0682851	0.0388131	0.0636924	0.0729745	0.113707	0.317195	1.05607
7	ADM-6005a_7	0.382109	0.0678588	0.0389113	0.0640267	0.0732265	0.113666	0.319045	1.05884
8	ADM-6005a_8	0.381185	0.068217	0.0390383	0.064036	0.0731137	0.113816	0.319457	1.05886
9	ADM-6005a_9	0.381249	0.0681775	0.0389637	0.0639798	0.0730421	0.113619	0.316589	1.05562
10	ADM-6005a_10	0.380373	0.0683098	0.0389339	0.063795	0.0728326	0.114285	0.318074	1.0566
11	ADM-6005a_11	0.381009	0.0680763	0.0390429	0.0639864	0.0729592	0.113997	0.318805	1.05788
12	ADM-6005a_12	0.381774	0.067932	0.038931	0.0639285	0.0727576	0.113903	0.317832	1.05706
13	ADM-6005a_13	0.381688	0.0681477	0.0388243	0.0640871	0.0729426	0.113803	0.318703	1.0582
14	ADM-6005a_14	0.38168	0.0678288	0.0389896	0.0639993	0.0728709	0.113778	0.318276	1.05742
15	ADM-6005a_15	0.382318	0.0682955	0.0387906	0.0640459	0.0731022	0.114217	0.318665	1.05943
16	ADM-6005a	0.3399	0.0664	0.0405	0.0683	0.0713	0.1055	0.3037	0.9956

We can use the describe(...) method from DataFrames to generate summary statistics.

describe(qdf[1:end-1,2:end], :mean, :std, :min, :max)

8×5 DataFrame

Row	variable	mean	std	min	max
	Symbol	Float64	Float64	Float64	Float64
1	O	0.381231	0.000704508	0.379643	0.382318
2	Al	0.0681017	0.000172422	0.0678288	0.0683536
3	Si	0.0388866	0.000113223	0.0386646	0.0390429
4	Ca	0.0639543	0.000110957	0.0636924	0.0640871
5	Ti	0.0730139	0.000153452	0.0727576	0.0733595
6	Zn	0.113973	0.0002319	0.113619	0.114285
7	Ge	0.318348	0.000845766	0.316589	0.319517
8	Total	1.05751	0.00106329	1.05562	1.05943

Or we can take a closer look at the data from one spectrum.

asa(DataFrame, qrs[1])

7×14 DataFrame

Row	Label	Element	Standard	Xrays	C	ΔC	k	Δk	g	Z	A	F	c	gZAFc
	String	String	String	String	Float64	Float64	Float64?	Float64?	Float64?	Float64?	Float64?	Float64?	Float64?	Float64?
1	ADM-6005a_1	Ti	Ti	Ti K-L3 + 3 others	0.07336	0.00012	0.0643276	0.000103282	1.0	0.925634	0.947328	1.0	1.0	0.876879
2	ADM-6005a_1	Al	Al	Al K-L3 + 3 others	0.068022	0.00012	0.0280766	4.99883e-5	1.0	1.03396	0.398685	1.0013	1.0	0.412758
3	ADM-6005a_1	Ge	Ge	Ge K-L3 + 1 other	0.31885	0.00064	0.263479	0.000525419	1.0	0.831431	0.993868	1.0	1.0	0.826333
4	ADM-6005a_1	Ca	CaF2	Ca K-L3 + 3 others	0.06395	8.9e-5	0.121389	0.000168661	1.0	1.04312	0.926501	1.00822	1.0	0.974395
5	ADM-6005a_1	Zn	Zn	Zn K-L3 + 1 other	0.11426	0.00028	0.111712	0.000272437	1.0	0.879367	0.999501	1.11233	1.0	0.977661
6	ADM-6005a_1	Si	SiO2	Si K-L3 + 3 others	0.038828	9.1e-5	0.0530552	0.000124176	1.0	1.11012	0.575032	1.00057	1.0	0.63872
7	ADM-6005a_1	O	SiO2	O K-L3 + 1 other	0.38076	0.00053	0.487558	0.000672807	1.0	1.10908	0.614952	0.999868	1.0	0.681942

Associated with each spectrum are a collection of properties. These properties are often read from the spectrum file but can also be assigned manually.

NeXLCore.properties(sp)

Dict{Symbol, Any} with 11 entries:
  :Owner           => "Bruker Nano"
  :RealTime        => 112.108
  :BeamEnergy      => 20000.0
  :Title           => "Bruker Nano spectrum Acquisition"
  :Elevation       => 0.698132
  :LiveTime        => 100.001
  :Filename        => "c:\\Users\\nritchie\\Desktop\\IUMAS\\data\\exp_raw\\ADM6…
  :ProbeCurrent    => 5.0
  :TakeOffAngle    => 0.698132
  :Name            => "ADM-6005a_1"
  :AcquisitionTime => DateTime("2019-07-12T09:33:00")

Properties are identified with a Symbol which is represented by a colon ':' plus a name. There are many predefined spectrum properties but you can also define your own to associate custom data with spectra.

sp[:BeamEnergy], sp[:ProbeCurrent], sp[:LiveTime], sp[:TakeOffAngle], dose(sp)

(20000.0, 5.0, 100.001, 0.6981317007977318, 500.005)

This is one way to index spectra to extract data from the spectrum. It is also possible to extract channel count data using various different types as indices. To demonstrate this, we will use Integer, AbstractFloat or CharXRay types to index the same channel in the spectrum - the channel associated with the Ca K-L3 peak.

channel(n"Ca K-L3", sp), channel(Float64, n"Ca K-L3", sp), channel(energy(n"Ca K-L3"), sp), channel(Float64, energy(n"Ca K-L3"), sp)

(833, 833.384891053903, 833, 833.384891053903)

In the first case, we index the channel directly by channel index. In the second case, we use a floating point number which is assumed to represent an energy to index the same channel. Finally, we use a CharXRay to index the same channel.

sp[833], sp[energy(n"Ca K-L3")], sp[n"Ca K-L3"]

(18042.0, 18042.0, 18042.0)

Often it is useful to be able to determine which of a collection of spectra collected from a single material under similar conditions are similar to one another. The notion being that the 'best' spectra are those that are most similar. These can then be summed together to produce a single spectrum that best represents the material. The findsimilar(...) method extracts the similar spectra from a list and removes outliers.

plot(sum(findsimilar(specs, refs.detector, n"O")), klms=[n"O", n"Al", n"Si", n"Ca", n"Ti", n"Zn", n"Ge"])

The similarity is determined by comparing each spectrum with the sum of the other spectra and calculating a score that respects count statistics. Similar spectra have a similarity(...) score of approximately unity.

DataFrame(Name=name.(specs), S1=NeXLSpectrum.similarity(specs, refs.detector, adm), S2=NeXLSpectrum.similarity(specs), Counts=integrate.(specs))

15×4 DataFrame

Row	Name	S1	S2	Counts
	String	Float64	Float64	Float64
1	ADM-6005a_1	0.861481	1.04111	6.81189e6
2	ADM-6005a_2	0.852062	0.970497	6.81126e6
3	ADM-6005a_3	0.854675	0.99976	6.81006e6
4	ADM-6005a_4	0.854278	0.980264	6.81625e6
5	ADM-6005a_5	0.89041	0.980602	6.80921e6
6	ADM-6005a_6	0.890928	0.962467	6.8086e6
7	ADM-6005a_7	0.841213	0.976628	6.81929e6
8	ADM-6005a_8	0.778826	0.971166	6.81616e6
9	ADM-6005a_9	0.83867	1.01652	6.816e6
10	ADM-6005a_10	0.847391	1.00353	6.81184e6
11	ADM-6005a_11	0.861667	0.975445	6.81146e6
12	ADM-6005a_12	0.823105	1.01421	6.81786e6
13	ADM-6005a_13	0.814398	0.974283	6.81113e6
14	ADM-6005a_14	0.777566	0.972348	6.81502e6
15	ADM-6005a_15	0.780707	0.942442	6.81972e6

HyperSpectra with NeXLSpectrum

A HyperSpectrum represents a multi-dimensional array of point spectra. NeXLSpectrum can handle a arbitrary number of dimensions like 1-D (linescans), 2-D (area scans) or higher dimensions.

There are currently three ways to load a hyperspectrum.

• From a Lispix-style RPL/RAW file pair
• From a SEMantics-style PTZ file
• From a HyperSpy-style HDF5 file

We will use the DataDeps library to download the hyperspectrum data on demand from the NIST data website. You will need to be connected to the Internet.

# DataDeps is a utility for downloading data on demand from a URL
using DataDeps
# Where do I want to put the data?
ENV["DATADEPS_LOAD_PATH"] = joinpath(datadir(), "exp_raw")
ENV["DATADEPS_ALWAYS_ACCEPT"]="true"
# Register the data sets using the names "MnDeepSeaNodule" and "MnDeepSeaNoduleStandards"
register(DataDep("MnDeepSeaNodule",
    """
    Dataset:       Deep Sea Manganese Nodule
    Acquired by:   Nicholas W.M. Ritchie
    License:       CC-SA 3.0
    """,
    raw"https://data.nist.gov/od/ds/mds2-2467/MnNodule.tar.gz",
    "5b5b6623b8f4daca3ff3073708442ac5702ff690aa12668659875ec5642b458d",
    post_fetch_method=DataDeps.unpack
));


register(DataDep("MnDeepSeaNoduleStandards",
    """
    Dataset:       Standard Spectra for Deep Sea Manganese Nodule Dataset
    Acquired by:   Nicholas W.M. Ritchie
    License:       CC-SA 3.0
    """,
    raw"https://data.nist.gov/od/ds/mds2-2467/MnNodule_Standards.tar.gz",
    "69283ba72146932ba451e679cf02fbd6b350f96f6d012d50f589ed9dd2e35f1a",
    post_fetch_method=DataDeps.unpack
));

The data is in RPL/RAW format - a format designed by David Bright at NIST and available from many EDS vendor's software. In addition to the data in the RPL/RAW format, we also need to provide spectrum meta-data and the detector energy scale.

raw = readrplraw(joinpath(datadep"MnDeepSeaNodule","map[15]"))
les = LinearEnergyScale(0.0, 10.0)
props = Dict{Symbol,Any}(
    :LiveTime => 0.72*4.0*18.0*3600.0/(1024.0*1024.0),
    :BeamEnergy => 20.0e3,
    :TakeOffAngle => deg2rad(35.0),
    :ProbeCurrent => 1.0,
    :Name => "Deep Sea Mn Nodule",
)
hs = HyperSpectrum(les, props, raw, fov = (0.2, 0.2))

1024 × 1024 HyperSpectrum{UInt16,(:Y, :X)}[Deep Sea Mn Nodule), 0.0 + 10.0⋅ch eV, 2048 ch]

It is easy to generate crude elemental maps from HyperSpectrum structs. These are simple ROI maps constructed by summing a range of channels around the central channel for the specified X-ray transition.

hs[n"Mn K-L3"]

Much like spectra, hyperspectra have properties. However, the same set of properties apply to all spectra within a hyperspectrum. There is one exception, :LiveTime, which can be an array of the same dimensionality as the hyperspectrum to represent a unique live-time per pixel.

NeXLCore.properties(hs)

Dict{Symbol, Any} with 5 entries:
  :Name         => "Deep Sea Mn Nodule"
  :BeamEnergy   => 20000.0
  :LiveTime     => 0.177979
  :TakeOffAngle => 0.610865
  :ProbeCurrent => 1.0

# This speeds up the processing by binning a 1024 x 1024 hyperspectrum to 1024/block_size x 1024/block_size.
block_size = 1
hs= block_size > 1 ? block(hs, (block_size, block_size)) : hs

1024 × 1024 HyperSpectrum{UInt16,(:Y, :X)}[Deep Sea Mn Nodule), 0.0 + 10.0⋅ch eV, 2048 ch]

Unfortunately, ROI maps suffer from many shortcomings including

• not being background corrected to eliminate the continuum signal
• not being scaled for differences in generation efficiency between different characteristic X-rays.

While they are convenient as a first glimse at the data, they can be very deceptive and should rarely be included in reports.

Instead, it is better to fit the point spectra within the hyperspectrum using measured references.

hs_elms = [ n"Ag", n"Al", n"Ba", n"C", n"Ca", n"Ce", n"Cr", n"Cu", n"Fe", n"S", n"P", n"K", n"Mg", n"O", n"Mn", n"Na", n"Cl", n"Ni", n"Si", n"Ti", n"Zn" ]
plot(maxpixel(hs), klms = hs_elms, xmax=10.0e3)

print(symbol.(sort(hs_elms)))

["C", "O", "Na", "Mg", "Al", "Si", "P", "S", "Cl", "K", "Ca", "Ti", "Cr", "Mn", "Fe", "Ni", "Cu", "Zn", "Ag", "Ba", "Ce"]

refs = references( [
        reference(n"C", joinpath(datadep"MnDeepSeaNoduleStandards", "C std.msa")),
        reference(n"O", joinpath(datadep"MnDeepSeaNoduleStandards", "MgO std.msa")),
        reference(n"Na", joinpath(datadep"MnDeepSeaNoduleStandards", "NaCl std.msa")),
        reference(n"Mg", joinpath(datadep"MnDeepSeaNoduleStandards", "Mg std.msa")),
        reference(n"Al", joinpath(datadep"MnDeepSeaNoduleStandards", "Al std.msa")),
        reference(n"Si", joinpath(datadep"MnDeepSeaNoduleStandards", "Si std.msa")),
        reference(n"P", joinpath(datadep"MnDeepSeaNoduleStandards", "GaP std.msa")), 
        reference(n"S", joinpath(datadep"MnDeepSeaNoduleStandards", "FeS2 std.msa")), 
        reference(n"Cl", joinpath(datadep"MnDeepSeaNoduleStandards", "NaCl std.msa")), 
        reference(n"K", joinpath(datadep"MnDeepSeaNoduleStandards", "KBr std.msa")), 
        reference(n"Ca", joinpath(datadep"MnDeepSeaNoduleStandards", "CaF2 std.msa")), 
        reference(n"Ti", joinpath(datadep"MnDeepSeaNoduleStandards", "Ti std.msa")), 
        reference(n"Cr", joinpath(datadep"MnDeepSeaNoduleStandards", "Cr std.msa")), 
        reference(n"Mn", joinpath(datadep"MnDeepSeaNoduleStandards", "Mn std.msa")), 
        reference(n"Fe", joinpath(datadep"MnDeepSeaNoduleStandards", "Fe std.msa")), 
        reference(n"Ni", joinpath(datadep"MnDeepSeaNoduleStandards", "Ni std.msa")), 
        reference(n"Cu", joinpath(datadep"MnDeepSeaNoduleStandards", "Cu std.msa")), 
        reference(n"Zn", joinpath(datadep"MnDeepSeaNoduleStandards", "Zn std.msa")), 
        reference(n"Ag", joinpath(datadep"MnDeepSeaNoduleStandards", "Ag std.msa")), 
        reference(n"Ba", joinpath(datadep"MnDeepSeaNoduleStandards", "BaF2 std.msa"))     
    ], 132.0)

asa(DataFrame, refs)

[ Info: A material containing Ba and F is not a suitable reference for "Ba M5-N3 + 16 others" due to a peak interference.

33×9 DataFrame

8 rows omitted

Row	Spectrum	Beam Energy (keV)	Probe Current (nA)	Live Time (s)	Material	Lines	ROI	P-to-B	S-to-N
	SubStrin…	Float64	Float64	Float64	Material…	Array…	UnitRang…	Float64	Float64
1	C std	20.0	0.97372	1184.6	C[C=1.0000,1.90 g/cm³]	C K-L3 + 1 other	16:40	24.143	15279.7
2	MgO std	20.0	0.9748	1161.48	MgO[Mg=0.6030,O=0.3970,5.00 g/cm³]	O K-L3 + 1 other	39:66	12.7889	8706.54
3	NaCl std	20.0	0.97454	1156.51	NaCl[Na=0.3934,Cl=0.6066,5.00 g/cm³]	Na K-L3 + 1 other	89:120	6.21839	9555.21
4	Mg std	20.0	0.97475	1149.05	Mg[Mg=1.0000,1.74 g/cm³]	Mg K-L3 + 1 other	110:142	17.4471	34147.0
5	Al std	20.0	0.97396	1151.25	Al[Al=1.0000,1.00 g/cm³]	Al K-L3 + 3 others	132:169	19.6389	36840.4
6	Si std	20.0	0.97465	1149.58	Si[Si=1.0000,2.95 g/cm³]	Si K-L3 + 3 others	157:198	25.0393	40461.5
7	GaP std	20.0	0.97451	1161.35	GaP[P=0.3076,Ga=0.6924,5.00 g/cm³]	P K-L3 + 3 others	184:230	8.27172	9393.98
8	FeS2 std	20.0	0.97334	1160.73	FeS2[S=0.5345,Fe=0.4655,5.00 g/cm³]	S K-L3 + 3 others	212:264	16.8388	21532.6
9	NaCl std	20.0	0.97454	1156.51	NaCl[Na=0.3934,Cl=0.6066,5.00 g/cm³]	Cl K-L3 + 3 others	243:300	23.512	25791.1
10	KBr std	20.0	0.97392	1147.26	KBr[Br=0.6714,K=0.3286,5.00 g/cm³]	K K-L3 + 3 others	310:379	7.04575	9501.98
11	CaF2 std	20.0	0.97401	1167.54	CaF2[Ca=0.5133,F=0.4867,3.18 g/cm³]	Ca K-L3 + 3 others	347:422	17.5274	19125.9
12	Ti std	20.0	0.9752	1160.26	Ti[Ti=1.0000,5.00 g/cm³]	Ti L3-M5 + 13 others	28:65	4.35094	3026.39
13	Ti std	20.0	0.9752	1160.26	Ti[Ti=1.0000,5.00 g/cm³]	Ti K-L3 + 3 others	427:516	20.5636	26561.6
⋮	⋮	⋮	⋮	⋮	⋮	⋮	⋮	⋮	⋮
22	Fe std	20.0	0.97436	1164.66	Fe[Fe=1.0000,7.87 g/cm³]	Fe K-M3 + 3 others	680:732	3.77854	3010.53
23	Ni std	20.0	0.97258	1164.08	Ni[Ni=1.0000,5.00 g/cm³]	Ni L3-M5 + 13 others	62:108	10.0052	11386.8
24	Ni std	20.0	0.97258	1164.08	Ni[Ni=1.0000,5.00 g/cm³]	Ni K-L3 + 1 other	718:778	16.0413	14413.1
25	Ni std	20.0	0.97258	1164.08	Ni[Ni=1.0000,5.00 g/cm³]	Ni K-M3 + 3 others	799:855	3.18328	2401.56
26	Cu std	20.0	0.97242	1159.85	Cu[Cu=1.0000,8.90 g/cm³]	Cu L3-M5 + 13 others	69:117	15.3703	19251.1
27	Cu std	20.0	0.97242	1159.85	Cu[Cu=1.0000,8.90 g/cm³]	Cu K-L3 + 1 other	773:836	14.0936	12296.1
28	Cu std	20.0	0.97242	1159.85	Cu[Cu=1.0000,8.90 g/cm³]	Cu K-M3 + 3 others	862:920	2.93067	2123.89
29	Zn std	20.0	0.97292	1157.03	Zn[Zn=1.0000,5.00 g/cm³]	Zn L3-M5 + 13 others	76:126	17.3497	23748.8
30	Zn std	20.0	0.97292	1157.03	Zn[Zn=1.0000,5.00 g/cm³]	Zn K-L3 + 1 other	831:896	12.5069	10519.0
31	Zn std	20.0	0.97292	1157.03	Zn[Zn=1.0000,5.00 g/cm³]	Zn K-M3 + 3 others	928:988	2.67558	1862.94
32	Ag std	20.0	0.98647	921.028	Ag[Ag=1.0000,5.00 g/cm³]	Ag L3-M5 + 25 others	247:393	5.28945	11615.2
33	BaF2 std	20.0	0.98986	1171.3	BaF2[Ba=0.7833,F=0.2167,5.00 g/cm³]	Ba L3-M5 + 29 others	377:617	2.85456	7169.28

Now we will fit the references to the hyperspectrum unknown. This is simple enough:

kratios_fast = fit_spectrum(hs, refs, mode = :Fast)

This is time consuming so once we've done it, we want to store the result in a file and reload the result rather than recalculate it. DrWatsons provides a mechanism to do this based on a function produce_or_load(....). You specify where to put the data and it builds a filename based on the prefix, suffix and the configuration paramters in @dict(mode, x_dim, y_dim). The suffix specifies that the data is written using the JLD2 library in HDF5 format.

# kratios_fast = @time fit_spectrum(hs, refs, mode = :Fast)  # Single threaded took 92 seconds

using FileIO, Parameters
mode = :Fast
x_dim, y_dim = size(hs)
data, file = produce_or_load(
        joinpath(datadir(),"exp_pro"), 
        @dict(mode, x_dim, y_dim),
        prefix="kratios", suffix="jld2"
    ) do config
        Dict("kratios" => @time fit_spectrum(hs, refs, mode = mode))
end
@show file
kratios_fast = data["kratios"]

file = "c:\\Users\\nritchie\\Desktop\\IUMAS\\data\\exp_pro\\kratios_mode=Fast_x_dim=1024_y_dim=1024.jld2"

33-element Vector{KRatios}:
 k[C, C K-L3 + 1 other] = Float64[ (1024, 1024) ]
 k[MgO, O K-L3 + 1 other] = Float64[ (1024, 1024) ]
 k[NaCl, Na K-L3 + 1 other] = Float64[ (1024, 1024) ]
 k[Mg, Mg K-L3 + 1 other] = Float64[ (1024, 1024) ]
 k[Al, Al K-L3 + 3 others] = Float64[ (1024, 1024) ]
 k[Si, Si K-L3 + 3 others] = Float64[ (1024, 1024) ]
 k[GaP, P K-L3 + 3 others] = Float64[ (1024, 1024) ]
 k[FeS2, S K-L3 + 3 others] = Float64[ (1024, 1024) ]
 k[NaCl, Cl K-L3 + 3 others] = Float64[ (1024, 1024) ]
 k[KBr, K K-L3 + 3 others] = Float64[ (1024, 1024) ]
 k[CaF2, Ca K-L3 + 3 others] = Float64[ (1024, 1024) ]
 k[Ti, Ti L3-M5 + 13 others] = Float64[ (1024, 1024) ]
 k[Ti, Ti K-L3 + 3 others] = Float64[ (1024, 1024) ]
 ⋮
 k[Fe, Fe K-M3 + 3 others] = Float64[ (1024, 1024) ]
 k[Ni, Ni L3-M5 + 13 others] = Float64[ (1024, 1024) ]
 k[Ni, Ni K-L3 + 1 other] = Float64[ (1024, 1024) ]
 k[Ni, Ni K-M3 + 3 others] = Float64[ (1024, 1024) ]
 k[Cu, Cu L3-M5 + 13 others] = Float64[ (1024, 1024) ]
 k[Cu, Cu K-L3 + 1 other] = Float64[ (1024, 1024) ]
 k[Cu, Cu K-M3 + 3 others] = Float64[ (1024, 1024) ]
 k[Zn, Zn L3-M5 + 13 others] = Float64[ (1024, 1024) ]
 k[Zn, Zn K-L3 + 1 other] = Float64[ (1024, 1024) ]
 k[Zn, Zn K-M3 + 3 others] = Float64[ (1024, 1024) ]
 k[Ag, Ag L3-M5 + 25 others] = Float64[ (1024, 1024) ]
 k[BaF2, Ba L3-M5 + 29 others] = Float64[ (1024, 1024) ]

The result of fit_spectrum(...) is a set k-ratio maps. Which can be readily visualized and represent a more quantitative perspective on the spectrum data. The principle advantage being that the data is background corrected so that continuum is not mistaken for a small quantity of an element.

To visualize the k-ratios, it is best to pick one k-ratio per element using optimizeks(...) and then normalize the k-ratios on a point-by-point basis using normalizek(...). This ensures that all the k-ratios are between 0 and 1. The function asa(ElementalMap, ...) facilitates this process by converting a Vector{KRatios} into a dictionary of images indexed by Element instances.

using Colors
imgs = asa(ElementalMap, kratios_fast, Gray)
imgs[n"Mn"]

We can perform matrix correction on the Vector{KRatios} using the quantify(...) method. It returns a Materials struct which is a memory efficient way of representing a multi-dimensional array of Material.

# quant_fast=quantify(kratios_fast, name=hs[:Name], ty=Float32) # Takes ~80 minute for 1024 x 1024 (~5 ms per pixel)

data, file = produce_or_load(
        joinpath(datadir(),"exp_pro"), 
        @dict(mode, x_dim, y_dim),
        prefix="quantify", suffix="jld2"
    ) do config
        Dict("mass_fractions" => @time quantify(kratios_fast, name=hs[:Name], ty=Float32))
end
@show file
quant_fast = data["mass_fractions"]

file = "c:\\Users\\nritchie\\Desktop\\IUMAS\\data\\exp_pro\\quantify_mode=Fast_x_dim=1024_y_dim=1024.jld2"

Materials[Deep Sea Mn Nodule, 1024 × 1024 × (C, O, Na, Mg, Al, Si, P, S, Cl, K, Ca, Ti, Cr, Mn, Fe, Ni, Cu, Zn, Ag, Ba)]

The Materials struct can be indexed at a specific coordinate to extract the composition at that coordinate as a Material.

quant_fast[128,384]

Deep Sea Mn Nodule[128,384][Ba=0.0008,Ca=0.0087,Mg=0.0006,O=0.2713,Cl=0.0064,K=0.0008,Ti=0.0011,Ag=0.0017,C=1.0478,Na=0.0054,Si=0.0414,Cu=0.0088,Mn=0.0039,Al=0.0143,Fe=0.0092]

Using broadcast, we can apply Material functions to Materials objects. The results is an Array with the same shape but with the result contents.

at_ms=analyticaltotal.(quant_fast)

1024×1024 Matrix{Float64}:
 1.12114   0.931418  1.0184    1.12544   …  0.798097  0.798483  0.750225
 0.877755  0.939474  0.87016   0.839677     0.826642  0.753609  0.814797
 0.944509  0.982147  0.936352  0.894357     0.789687  0.802227  0.806136
 0.877553  0.834916  0.877479  0.952697     0.69093   0.722851  0.736526
 0.83982   0.831247  0.790591  0.944809     0.604645  0.658924  0.682592
 0.874638  0.908482  0.92161   0.851666  …  0.673269  0.714052  0.675014
 0.920448  0.973551  0.997805  0.919651     0.822391  0.687747  0.698407
 0.901042  0.892611  0.878813  0.943202     0.794712  0.749333  0.647348
 0.840059  0.901996  0.919389  0.944544     0.783919  0.788288  0.667246
 0.904216  0.947249  0.971246  0.89693      0.926894  0.825388  0.742284
 0.972421  1.02393   0.94819   0.948975  …  0.862409  0.826175  0.766345
 0.932931  0.945948  0.882228  0.975659     0.782198  0.80973   0.804723
 0.916943  0.905414  0.837847  0.824939     0.891919  0.883625  0.82066
 ⋮                                       ⋱                      
 0.882333  0.928941  0.937709  0.994533     0.965608  0.838502  0.799263
 1.00358   0.993153  0.931432  0.955147     0.736347  0.883015  0.900127
 1.02583   1.06478   0.964631  1.00421      0.840045  0.864325  0.949038
 1.03194   0.947343  0.85004   1.06743   …  0.912345  0.97687   0.922914
 1.03552   1.02994   1.01893   1.00077      0.987512  1.06054   1.09555
 1.0135    1.03027   0.980763  0.945134     0.809482  0.875999  1.08297
 1.10909   1.11128   1.03744   0.993881     0.602245  0.734092  0.860694
 1.15768   1.01753   1.01024   1.04317      0.517874  0.572694  0.701184
 0.989872  1.1088    1.00917   1.01493   …  0.520139  0.556505  0.810547
 1.0812    1.00858   0.999245  1.00088      0.606844  0.731831  0.94359
 0.911391  0.961544  0.924331  0.962723     0.745007  0.92867   0.979702
 0.982772  1.04914   1.00912   0.988079     0.78446   0.890835  0.926269

using Statistics
mean(at_ms), std(at_ms)

(1.0447547161174755, 0.1606245028098845)

To convert the mass-fractions to images, we need to ensure all mass-fractions are on the range [0,1]. We can do this by normalizing the individual points to an analytical total of unity.

quant_fast_norm=asnormalized(quant_fast)

Materials[N[Deep Sea Mn Nodule], 1024 × 1024 × (C, O, Na, Mg, Al, Si, P, S, Cl, K, Ca, Ti, Cr, Mn, Fe, Ni, Cu, Zn, Ag, Ba)]

Now let's visualize this. In Julia, it is trivial to convert matrices representing values on the range [0,1] to images.

We will extract the plane of data corresponding to an element by indexing it with an Element. Log3Band is a function that converts numbers between 0 and 1 to RGB values. The mapping is displayed below in the legend.

Log3Band.(quant_fast_norm[n"Ni"])

loadlegend("Log3BandBright.png")

The Ni elemental map can be seen to represent primarily values ranging from a few percent down to zero. Albeit, this spectrum image took 18 hours to collect but the depth of information might surprise many who are used to thinking of spectrum images as a crude tool.

Let's output various perspectives from each element to the 'plots' directory. The Gray function converts values on the range [0,1] to gray-scale values.

# Fast k-ratio maps
let imgs = asa(ElementalMap, kratios_fast, Log3Band) 
    for (el, img) in imgs
        save(joinpath(plotsdir(),"$(symbol(el)) - Fast Log3Band.png"), img)
    end
end
# Full k-ratio maps
let imgs = asa(ElementalMap, kratios_fast, Gray) 
    for (el, img) in imgs
        save(joinpath(plotsdir(),"$(symbol(el)) - Fast Gray.png"), img)
    end
end
# Full quantitative maps - Fast fit
begin
    for el in keys(quant_fast_norm)
        save(joinpath(plotsdir(),"$(symbol(el)) - Quant Fast Gray.png"), Gray.(quant_fast_norm[el]))
        save(joinpath(plotsdir(),"$(symbol(el)) - Quant Fast Log3Band.png"), Log3Band.(quant_fast_norm[el]))
    end
end

All of these results have been based on the mode=:Fast fit of the standard spectra to the hyperspectrum data.

Now we will perform a mode=:Full fit of the HyperSpectrum data. This takes a couple of orders of magnitude more time than the mode=:Fast fit. However, the :Full mode won't return negative k-ratios and, in general, performs a much more careful fit.

# kratios_full = @time fit_spectrum(hs, refs, mode = :Full) # Single threaded took 6132 seconds

mode = :Full
data, file = produce_or_load(
        joinpath(datadir(),"exp_pro"), 
        @dict(mode, x_dim, y_dim),
        prefix="kratios", suffix="jld2"
    ) do config
        Dict("kratios" => @time fit_spectrum(hs, refs, mode = mode))
end
@show file
kratios_full = data["kratios"]

file = "c:\\Users\\nritchie\\Desktop\\IUMAS\\data\\exp_pro\\kratios_mode=Full_x_dim=1024_y_dim=1024.jld2"

33-element Vector{KRatios}:
 k[C, C K-L3 + 1 other] = Float32[ (1024, 1024) ]
 k[MgO, O K-L3 + 1 other] = Float32[ (1024, 1024) ]
 k[NaCl, Na K-L3 + 1 other] = Float32[ (1024, 1024) ]
 k[Mg, Mg K-L3 + 1 other] = Float32[ (1024, 1024) ]
 k[Al, Al K-L3 + 3 others] = Float32[ (1024, 1024) ]
 k[Si, Si K-L3 + 3 others] = Float32[ (1024, 1024) ]
 k[GaP, P K-L3 + 3 others] = Float32[ (1024, 1024) ]
 k[FeS2, S K-L3 + 3 others] = Float32[ (1024, 1024) ]
 k[NaCl, Cl K-L3 + 3 others] = Float32[ (1024, 1024) ]
 k[KBr, K K-L3 + 3 others] = Float32[ (1024, 1024) ]
 k[CaF2, Ca K-L3 + 3 others] = Float32[ (1024, 1024) ]
 k[Ti, Ti L3-M5 + 13 others] = Float32[ (1024, 1024) ]
 k[Ti, Ti K-L3 + 3 others] = Float32[ (1024, 1024) ]
 ⋮
 k[Fe, Fe K-M3 + 3 others] = Float32[ (1024, 1024) ]
 k[Ni, Ni L3-M5 + 13 others] = Float32[ (1024, 1024) ]
 k[Ni, Ni K-L3 + 1 other] = Float32[ (1024, 1024) ]
 k[Ni, Ni K-M3 + 3 others] = Float32[ (1024, 1024) ]
 k[Cu, Cu L3-M5 + 13 others] = Float32[ (1024, 1024) ]
 k[Cu, Cu K-L3 + 1 other] = Float32[ (1024, 1024) ]
 k[Cu, Cu K-M3 + 3 others] = Float32[ (1024, 1024) ]
 k[Zn, Zn L3-M5 + 13 others] = Float32[ (1024, 1024) ]
 k[Zn, Zn K-L3 + 1 other] = Float32[ (1024, 1024) ]
 k[Zn, Zn K-M3 + 3 others] = Float32[ (1024, 1024) ]
 k[Ag, Ag L3-M5 + 25 others] = Float32[ (1024, 1024) ]
 k[BaF2, Ba L3-M5 + 29 others] = Float32[ (1024, 1024) ]

Let's add the :Full fit k-ratio data images to the 'plots' directory for comparison.

using Colors
let imgs = asa(ElementalMap, kratios_full, Log3Band) 
    for (el, img) in imgs
        save(joinpath(plotsdir(),"$(symbol(el)) - Full Log3Band.png"), img)
    end
end
let imgs = asa(ElementalMap, kratios_full, Gray) 
    for (el, img) in imgs
        save(joinpath(plotsdir(),"$(symbol(el)) - Full Gray.png"), img)
    end
end

Let's compare the results from the full fit with the results from the fast fit.

imgs_full = asa(ElementalMap, kratios_full, Log3Band)
els = sort([ keys(imgs_full)...])
print(symbol.(els))

["C", "O", "Na", "Mg", "Al", "Si", "P", "S", "Cl", "K", "Ca", "Ti", "Cr", "Mn", "Fe", "Ni", "Cu", "Zn", "Ag", "Ba"]

map( el->imgs_full[el], els)

(a vector displayed as a row to save space)

begin
    imgs_fast = asa(ElementalMap, kratios_fast, Log3Band)
    map( el->imgs_fast[el], els)
end

(a vector displayed as a row to save space)

Now let's quantify the :Full fit data. Performing the matrix correction is actually much slower than performing the :Full fit.

Again, the results are a Materials struct.

# quant_full = @time quantify(kratios_full, name=hs[:Name])

data, file = produce_or_load(
        joinpath(datadir(),"exp_pro"), 
        @dict(mode, x_dim, y_dim),
        prefix="quantify", suffix="jld2"
    ) do config
        Dict("mass_fractions" => @time quantify(kratios_full, name=hs[:Name], ty=Float32))
end
@show file
quant_full = data["mass_fractions"]

[ Info: File c:\Users\nritchie\Desktop\IUMAS\data\exp_pro\quantify_mode=Full_x_dim=1024_y_dim=1024.jld2 does not exist. Producing it now...

4467.479611 seconds (32.22 G allocations: 7.521 TiB, 16.99% gc time, 0.03% compilation time: 49% of which was recompilation)

┌ Warning: The Git repository ('c:\Users\nritchie\Desktop\IUMAS') is dirty! Appending -dirty to the commit ID.
└ @ DrWatson C:\Users\nritchie\.julia\packages\DrWatson\JACNB\src\saving_tools.jl:64

file = "c:\\Users\\nritchie\\Desktop\\IUMAS\\data\\exp_pro\\quantify_mode=Full_x_dim=1024_y_dim=1024.jld2"

[ Info: File c:\Users\nritchie\Desktop\IUMAS\data\exp_pro\quantify_mode=Full_x_dim=1024_y_dim=1024.jld2 saved.

Materials[Deep Sea Mn Nodule, 1024 × 1024 × (C, O, Na, Mg, Al, Si, P, S, Cl, K, Ca, Ti, Cr, Mn, Fe, Ni, Cu, Zn, Ag, Ba)]

map(el->Log3Band.(quant_full[el]), els)

(a vector displayed as a row to save space)

Clearly, the light element maps are where we see the influence of matrix correction. When X-ray absorption is small, the k-ratio is generally a good approximation of the mass-fraction. However, for low energy X-rays, the absorption can be strong leading to a significant underestimation of the mass fraction. We see this particularly in the carbon data.

Now write these images to disk.

begin
    quant_full_norm=asnormalized(quant_full)
    for el in keys(quant_full_norm)
        save(joinpath(plotsdir(),"$(symbol(el)) - Quant Full Gray.png"), Gray.(quant_full_norm[el]))
        save(joinpath(plotsdir(),"$(symbol(el)) - Quant Full Log3Band.png"), Log3Band.(quant_full_norm[el]))
    end
end

quant_full[n"Mn"]

1024×1024 Matrix{Float32}:
 0.223394    0.311174   0.332411    …  0.192086    0.18319     0.182768
 0.269441    0.277169   0.307894       0.187049    0.187401    0.198357
 0.27579     0.272186   0.242913       0.1994      0.215164    0.195631
 0.284984    0.254272   0.251819       0.221909    0.19468     0.228718
 0.271912    0.248145   0.231546       0.181427    0.315283    0.155952
 0.00486168  0.235095   0.232646    …  0.209557    0.0161902   0.198351
 0.216475    0.192771   0.306901       0.200423    0.165684    0.218023
 0.220113    0.231561   0.285585       0.213188    0.22912     0.21971
 0.248034    0.252878   0.272362       0.19302     0.214149    0.281862
 0.24977     0.260708   0.239762       0.301234    0.185244    0.209922
 0.266883    0.271193   0.297616    …  0.165329    0.190385    0.211984
 0.301004    0.146325   0.274044       0.26669     0.218611    0.207211
 0.29647     0.303459   0.285447       0.265315    0.248976    0.217168
 ⋮                                  ⋱                          
 0.324508    0.324034   0.26046        0.00610759  0.00819175  0.0323414
 0.223967    0.298605   0.231759       0.247855    0.0136075   0.0366124
 0.267053    0.2395     0.00541237     0.00076621  0.0255185   0.0395083
 0.0377666   0.161325   0.092179    …  0.0         0.416347    0.00254732
 0.147561    0.097022   0.0636286      0.193515    0.00693751  0.00533547
 0.0941413   0.0659752  0.0677662      0.00869319  0.00985284  0.00891134
 0.101526    0.07201    0.104355       0.0264528   0.017331    0.00477545
 0.27833     0.129675   0.188148       0.036561    0.0274113   0.0151129
 0.15678     0.207637   0.274506    …  0.0463395   0.0424375   0.334446
 0.225777    0.146953   0.385326       0.069456    0.0334889   0.0160826
 0.208606    0.294549   0.346879       0.0603972   0.0310457   0.0142638
 0.220558    0.30014    0.321251       0.0684462   0.0361965   0.0130948

using Statistics
mean(analyticaltotal.(quant_full)), mean(analyticaltotal.(quant_fast))

(1.0397453436659276, 1.0447547161174755)

To explore the data, let's plot histograms of the mass fractions from each element.

colors = distinguishable_colors(length(els), colorant"light blue", lchoices=range(50, stop=100, length=15))
    
plot(
    ( layer(x=quant_full[el], Geom.histogram, Theme(default_color=colors[i]), alpha=[0.6]) for (i, el) in enumerate(els) )...,
    Guide.xlabel("Mass Fraction"), Guide.ylabel("Counts"), 
    Guide.manual_color_key("Element", symbol.(els), colors),
    Coord.cartesian(xmin=0.0, xmax=1.0, ymax=16.0e4)
)

plot(
    ( layer(x=quant_full[el], Geom.histogram, Theme(default_color=colors[i]), alpha=[0.6]) for (i, el) in enumerate(els) )...,
    Guide.xlabel("Mass Fraction"), Guide.ylabel("Counts"), 
    Guide.manual_color_key("Element", symbol.(els), colors),
    Coord.cartesian(xmin=0.0, xmax=0.05, ymax=16.0e4)
)

We can easily query the quantified data using broadcast syntax to create BitMatrix based on a boolean comparison. To determine which pixels have a mass-fraction of Si > 5% we create a mask. In this BitMatrix mask, 1 represents a true comparison and 0 a false comparison.

mask_si = quant_full[n"Si"] .> 0.05

1024×1024 BitMatrix:
 0  0  0  1  0  1  1  1  1  0  0  0  0  …  0  0  0  0  0  0  0  0  1  1  0  0
 0  0  0  0  0  0  0  0  0  1  0  0  0     0  0  0  0  0  0  0  0  0  1  0  0
 0  0  0  0  0  0  0  0  0  0  0  0  0     0  0  0  0  0  0  0  0  0  1  0  0
 0  0  0  0  0  0  0  0  0  0  0  1  0     0  0  0  0  0  1  0  0  0  0  0  0
 0  0  0  0  0  0  0  0  0  0  0  0  0     0  0  0  0  0  0  1  0  0  0  0  1
 0  0  0  0  0  0  0  0  0  0  0  0  0  …  0  0  0  0  0  0  0  0  0  0  0  0
 0  1  1  0  0  0  0  0  0  0  0  0  0     1  0  0  0  0  0  0  0  0  0  0  0
 0  1  0  0  0  0  0  0  0  0  0  1  1     0  0  0  0  0  0  0  0  0  0  0  0
 0  0  0  1  1  0  0  0  0  0  1  1  1     0  0  0  0  0  0  0  0  0  0  0  0
 0  0  1  0  1  0  0  0  0  0  1  1  1     0  0  0  0  1  0  0  1  0  0  0  0
 0  0  0  0  0  1  0  0  0  0  0  1  1  …  0  0  0  0  0  0  0  1  1  1  0  0
 0  1  0  0  0  1  1  0  1  1  0  0  0     0  0  0  0  0  0  0  0  1  0  0  0
 0  0  0  0  0  1  1  0  0  0  0  0  0     0  0  0  0  0  0  0  0  0  0  0  0
 ⋮              ⋮              ⋮        ⋱           ⋮              ⋮        
 0  0  0  0  1  1  1  1  1  1  1  1  0     1  1  1  1  1  1  1  1  1  1  1  1
 0  0  0  1  0  1  1  1  1  1  1  1  1     1  1  1  1  1  1  1  1  0  0  1  1
 0  0  1  1  1  1  1  1  1  1  1  0  0     1  0  1  0  1  1  1  1  1  1  0  1
 1  1  1  0  0  1  1  1  1  0  1  1  0  …  1  0  0  1  0  0  1  1  1  1  0  1
 1  1  1  1  1  1  1  0  1  1  1  1  0     1  1  1  1  1  1  1  1  1  1  1  1
 1  1  1  1  1  1  0  0  0  0  1  0  1     1  1  1  1  0  1  1  1  1  1  0  0
 1  1  1  1  1  0  0  0  1  1  1  1  0     1  1  0  1  1  1  1  1  0  0  0  0
 0  1  1  0  0  0  0  0  0  0  0  0  0     1  1  1  1  1  1  1  1  1  1  0  0
 0  0  0  1  0  0  0  0  0  0  1  0  0  …  1  1  1  1  1  1  1  1  0  0  0  1
 0  1  1  0  0  0  0  0  0  0  0  0  0     0  1  0  1  1  0  1  1  1  1  1  1
 0  0  0  0  0  0  0  0  0  0  0  0  0     0  0  0  1  1  1  1  0  1  1  1  1
 0  0  0  1  1  1  0  0  0  0  0  0  0     0  0  0  0  0  1  0  0  1  1  1  1

Using similar syntax we can determine how many pixels have at least 50%, 10%, 5% and 1% of an element?

DataFrame(
    Element=symbol.(els), 
    P50=map(el->count(quant_full[el] .> 0.5),els), 
    P10=map(el->count(quant_full[el] .> 0.1),els), 
    P5=map(el->count(quant_full[el] .> 0.05),els), 
    P1=map(el->count(quant_full[el] .> 0.01),els)
)

20×5 DataFrame

Row	Element	P50	P10	P5	P1
	String	Int64	Int64	Int64	Int64
1	C	86704	720858	1019909	1045263
2	O	35574	1034995	1040636	1045908
3	Na	0	39	5515	603161
4	Mg	0	96	896	727196
5	Al	0	5380	39062	742418
6	Si	5	121297	270774	942104
7	P	0	213	653	2336
8	S	0	1	28	115253
9	Cl	0	0	1	23493
10	K	0	453	3768	269937
11	Ca	0	1190	5723	809920
12	Ti	0	159	469	4871
13	Cr	0	0	3	121
14	Mn	184	863934	918021	990386
15	Fe	33	182310	506314	960971
16	Ni	2	10	15	543173
17	Cu	0	6	11	416359
18	Zn	2	75	214	85702
19	Ag	0	1	12	17231
20	Ba	0	212	1064	67902

A mask can then be applied to extract and sum the requisite spectra within the hyperspectrum.

plot( sum(hs, quant_full[n"Si"] .> 0.05), klms=els, xmax=10.0e3)

Let's do something similar for Cu > 10%.

plot( sum(hs, quant_full[n"Cu"] .> 0.1), klms=els, xmax=10.0e3)

This is just a flavor of what you can do with spectra and hyperspectra using Julia, the Julia library infrastructure including the NeXL libraries. There are many machine learning, chemometric, image analysis and other libraries that can be readily applied.